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Relativistic Heavy Ion Collider

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10,000 quarks & gluon in fireball. RHIC at Brookhaven National Laboratory ... energetic particles, heavy particle (charm) probe interior of expanding fireball. ... – PowerPoint PPT presentation

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Title: Relativistic Heavy Ion Collider


1
Relativistic Heavy Ion Collider
2
Quarks and Gluons
  • Quarks and gluons are the constituents of protons
    neutrons, atomic nuclei, neutron stars
    (pulsars), and the very early universe.
  • A proton has three quarks (uud) plus a
    fluctuating cloud of quark anti-quark pairs and
    gluons.
  • E mc2. In energy units, the mass of the proton
    is 938 MeV/c2.
  • The 3 bare quarks of the proton contribute only
    15 MeV/c2 to the mass of the proton.
  • One of the central goals of particle physics is
    to find the origin of this 1.5 of the mass of
    the proton.
  • The central goal of Jefferson Lab, and the
    Relativistic Heavy Ion Collider is to understand
    the origin of the other 98.5 of the mass of the
    proton.
  • This is also 98.5 of the mass of the visible
    matter of the universe.

3
Quark and Gluon waves
  • Any wave is described by its wavelength l and
    frequency f1/T.
  • Energy density carried by a wave is proportional
    to amplitude squared.
  • Quantum waves
  • Momentum l / h
  • Energy f h
  • Relativity Emc2 (p0)
  • E2 (pc)2 (mc2)2

4
Quark and gluon waves interact by creation and
annihilation
  • Quark wave ? Quark Gluon waves
  • Anti-Quark wave ? Anti-Quark Gluon waves
  • QuarkAnti-Quark ? Gluon wave
  • Gluon wave ? Quark Anti-Quark waves
  • l1 l2 l3
  • f1 f2 f3
  • These conditions violate the mass constraint E2
    - (pc)2 (mc2)2
  • Quarks gluons almost massless.
  • The Off-mass-shell waves only propagate for a
    time h/(E-pc)

5
The Jefferson Lab Strategy
  • Focus the simplest systems
  • Protons, Deuterons, Helium,
  • Study with a well understood microscope
  • Short wavelength Photon and Electron waves
  • Study at short distance inside the proton,
  • QCD (better) understood.

6
The Relativistic Heavy Ion Collider (RHIC)
strategy
  • Symmetric Au-Au collisions at high energy
  • Total energy 2A200 GeV, A 197 nucleons
  • Apply Thermodynamics to nuclear matter at high
    temperature
  • Recreate the conditions of the early universe
  • Look for phase transitions between hadronic
    matter (protons, neutrons, pions) and
    Quark-Gluon Plasma.

7
Create a little bang in the lab!
Use accelerators to reach highest energy vBEAM
0.99995 x speed of light at RHIC center of mass
energy ?s 200 GeV/nucleon Use heaviest beams
possible maximum volume of plasma 10,000 quarks
gluon in fireball
8
RHIC at Brookhaven National Laboratory
RHIC is first dedicated heavy ion collider 10
times the energy previously available!
9
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10
4 complementary experiments
11
Black Body Radiation
Radiated Power
  • Peak frequency proportional to Temperature
  • fpeak 2.82 kT/ h
  • Total power radiated per unit area

12
Cosmic Microwave BackgroundNASA/WMAP Science
Team
Red to Blue, T 2.725?0.001 K
13
Black Body Radiation from Relativistic Heavy Ion
collisions
  • At low temperature, neutrons and protons are
    boiled out of the nuclei
  • If kT gt mc2, particles are created (mostly pions,
    mc2 140 MeV).
  • The Black Body radiation depends upon the number
    of degrees of freedom
  • Low temperature 2 x 2 (protonneutron) x spin
  • High temperature (3 x 3 8)x 2 3 quark flavors
    times 3 quark colors times 8 gluon color
    anti-color states.

14
In AA QCD in non-perturbative regime
Lattice
e Energy density
T/Tc
Physics is soft Lattice QCD says Create these
conditions to look for new physics
15
Is the energy density high enough?
PRL87, 052301 (2001)
16
history of heavy ion collisions
high e, pressure builds up
g, g? ee-, mm-
p, K, p, n, f, L, D, X, W, d,
Real and virtual photons from q scattering
sensitive to the early stages. Probe also with q
and g produced early, passing through the
medium on their way out.
Hadrons reflect medium properties when inelastic
collisions stop (chemical freeze-out).
17
Particle production (lots!)
sum particles under the curve, find 5000
charged particles in collision final state (6200
in 200 A GeV central AuAu)
In initial volume Vnucleus Rescattering should
be important!
18
Measuring Impact Parameter
  • On an event-event basis, collisions are highly
    localized (but random).
  • Multiplicity of particles in a set of reference
    detectors is a good surrogate for impact
    parameter
  • Higher multiplicity for central collisions
  • Sharp cutoff for grazing collisions.
  • Extreme forward detectors measure low
    multiplicity for central collisions.

19
More evidence for equilibrated final state
Observed hadron ratios in agreement with thermal
ratios! T(chemical freeze-out) 175 MeV
20
Early state? a barometer called elliptic flow
Origin spatial anisotropy of the system when
created, followed by multiple scattering of
particles in the evolving system spatial
anisotropy ? momentum anisotropy
v2 2nd harmonic Fourier coefficient in
azimuthal distribution of particles with respect
to the reaction plane
21
a unique probe for physics of hot medium
Probe Jets from hard scattered quarks Observed
via fast leading particles or azimuthal
correlations between the leading particles
  • But, before they create jets, the scattered
    quarks radiate energy ( GeV/fm) in the colored
    medium
  • decreases their momentum (fewer high pT
    particles)
  • kills jet partner on other side
  • jet quenching

22

Au-Au ?s 200 GeV high pT suppression!
nucl-ex/0304022
Au-Au nucl-ex/0304022
23
jet correlations AuAu vs pp
STAR PRL 90, 082302 (2003)
Peripheral Au Au
Central Au Au
24
Experiments show NO suppression in dAu!
PHENIX Preliminary p0
STAR Preliminary
25
?0 RAA vs. predictions
Theoretical predictions dAu I. Vitev,
nucl-th/0302002 and private communication.
AuAu I. Vitev and M. Gyulassy, hep-ph/0208108,
to appear in Nucl. Phys. A M. Gyulassy, P. Levai
and I. Vitev, Nucl. Phys. B 594, p. 371 (2001).
Initial state mult. scatt.,shadowing final
state dE/dx (AuAu) Also Kopeliovich, et al
(PRL88, 232303,2002) predict RpA1.1 max at
pT2.5 GeV projectile as color dipole
anti-shadowing
shadowing
26
Conclusions
  • Huge multiplicity of particles in each event
    allows approach to statistical (thermodynamic)
    treatment
  • Many ideas are semi-classical.
  • Extreme energetic particles, heavy particle
    (charm) probe interior of expanding fireball.
  • Correlations in multiparticle emission allow more
    detailed image of events.
  • Theory is mostly crude, but trying to understand
    essential dynamics.

27
Centrality Dependence
Au Au Experiment
d Au Control
  • Dramatically different and opposite centrality
    evolution of AuAu experiment from dAu control.
  • Jet Suppression is clearly a final state effect.
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